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Journal ArticleDOI

Spin-glass behavior of AFe4Al8 (A=Th,U,Np) intermetallics.

TLDR
The freezing temperature under high external fields is labels as the upper limit of the SG temperature, and indicates a true thermodynamic phase transition; the cusp in the ac susceptibility is not necessarily a confirmation for the establishment of a SG state.
Abstract
Combined ac- and dc-susceptibility, neutron-diffraction, and M\"ossbauer studies of ${\mathrm{UFe}}_{4}$${\mathrm{Al}}_{8}$, ${\mathrm{NpFe}}_{4}$${\mathrm{Al}}_{8}$, and ${\mathrm{ThFe}}_{4}$${\mathrm{Al}}_{8}$ argue for the establishment of a spin-glass (SG) state below ${\mathit{T}}_{\mathrm{SG}}$(B\ensuremath{\rightarrow}0)\ensuremath{\approxeq}130, 120, and 110 K, respectively. The SG temperature ${\mathit{T}}_{\mathrm{SG}}$(B) decreases with application of external magnetic field B. The ac susceptibility (${\mathrm{\ensuremath{\chi}}}_{\mathrm{ac}}$) shows a sharp cusp at ${\mathit{T}}_{\mathrm{SG}}$(B\ensuremath{\approxeq}0). The isothermal and thermoremanent magnetization differ markedly and show temperature-dependent irreversibilities below ${\mathit{T}}_{\mathrm{SG}}$(B). The M\"ossbauer spectra reveal onset of hyperfine splitting, indicating frozen spins below ${\mathit{T}}_{\mathrm{SG}}$(0). The neutron-diffraction studies of ${\mathrm{UFe}}_{4}$${\mathrm{Al}}_{8}$ and ${\mathrm{NpFe}}_{4}$${\mathrm{Al}}_{8}$ show that after switching off the external magnetic field greater than 3 T the U and Np momenta (2a site) are frozen parallel to the direction of the external field. We label the freezing temperature under high external fields ${\mathit{T}}_{\mathrm{OG}}$, and show that it serves as the upper limit of ${\mathit{T}}_{\mathrm{SG}}$(B) with ${\mathit{T}}_{\mathrm{SG}}$(B\ensuremath{\rightarrow}0)\ensuremath{\rightarrow}${\mathit{T}}_{\mathrm{OG}}$. For concentrated SG systems, ${\mathit{T}}_{\mathrm{SG}}$(0) is a reproducible value, independent of the observation time window, which indicates a true thermodynamic phase transition; the cusp in ${\mathrm{\ensuremath{\chi}}}_{\mathrm{ac}}$, however, is not necessarily a confirmation for the establishment of a SG state.

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Book ChapterDOI

Chapter 149 The ThMn12-Type compounds of rare earths and actinides: Structure, magnetic and related properties

TL;DR: In this article, the structure, magnetic, and related properties of the ThMn12-type compounds of rare earths and actinides are presented, and the magnetic coupling for these compounds is determined only for the AnFe4Al8 seiles in neutron diffraction (ND) experiment.
Journal ArticleDOI

The crystal and magnetic structures of intermetallic compounds

TL;DR: In this paper, the powder samples of (x = 4, 5 and 6) alloys have been measured by means of magnetization, Mossbauer effect, x-ray and neutron diffraction techniques in the temperature range 15 - 400 K.
Journal ArticleDOI

Neutron diffraction study of the ferrimagnetic structures of RFe5Al7 compounds with R = Tb, Dy, Ho, Er, Tm

TL;DR: In this article, the long range order of ternary RFe 5 Al 7 (R = Tb, Dy, Ho, Er, Tm) intermetallics of ThMn 12 -type structure is analyzed by neutron powder diffraction.
Journal ArticleDOI

High field magnetization of UAl12−xfex (4.0 ⩽= x ⩽= 4.8) intermetallic compounds

TL;DR: The magnetization of UAl 12−x Fe x intermetallic compounds at 4.2 K in magnetic fields up to 35 T has been studied on powder particles free to be oriented by the applied field and on particles fixed by frozen alcohol as discussed by the authors.
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